An Introduction to Stochastic PDEs I: The Cameron–Martin TheoremTextbook
Motivation
A stochastic partial differential equation is driven by noise that lives on an infinite-dimensional function space, and the first object one has to control is the law of that noise: a Gaussian measure on a separable Banach space. Martin Hairer's lecture notes An Introduction to Stochastic PDEs (arXiv:0907.4178) devote their first technical chapter (Section 4) to exactly this, because every later construction — stochastic convolutions, invariant measures for semilinear equations, the ergodic theory of the stochastic Navier–Stokes equations — is phrased against it.
The single structural fact that chapter produces is the Cameron–Martin theorem (Theorem 4.44, p. 31). It answers the question: in which directions may one translate an infinite-dimensional Gaussian measure without destroying its null sets? In finite dimensions the answer is "all of them", because Lebesgue measure is translation invariant. In infinite dimensions the admissible directions form a proper, and typically much smaller, Hilbert subspace — the Cameron–Martin space — and the translated measure is either equivalent to or mutually singular with it, with nothing in between. This dichotomy is the reason Girsanov-type changes of measure, Schilder-type large deviation rate functions, support theorems and Malliavin calculus all take the form they do.
Setting
Throughout, is a separable Banach space, its topological dual, and a Borel probability measure on .
is Gaussian (Definition 4.4, p. 19) if for every continuous linear functional the push-forward is a Gaussian measure on in the sense of Definition 4.1, i.e. has characteristic function ; the degenerate case , a Dirac mass, is included. It is centred if all these one-dimensional laws have mean zero, which is expressed here as .
For a centred Gaussian the covariance form (4.2, p. 20) is
It is well defined because is -integrable, and it is a bounded bilinear form (Corollary 4.14, p. 22).
The Cameron–Martin space (Definition 4.26, p. 27) is classically built as the completion of
under . This mission uses the equivalent intrinsic description of Exercise 4.38 (p. 29), which avoids the completion:
The supremum is taken in ; since is admissible whenever is, it equals over the same set. For write , .
Formalization targets
Goal — Theorem 4.44 (Cameron–Martin)
For a centred Gaussian measure on a separable Banach space and ,
Both implications are asserted: translation along a Cameron–Martin direction produces an absolutely continuous measure, and translation along any other direction does not (in fact it produces a mutually singular measure).
Milestones
The milestone list follows the route of Section 4.2:
- Exercise 4.38 — the supremum description agrees with Definition 4.26 on .
- Proposition 4.32 — with .
- Proposition 4.40 — every -limit of elements of has a centred Gaussian law whose variance is its own norm squared.
- Equation (4.14) — the explicit density of the shifted measure, for .
- The total-variation separation bound used in the converse half of Theorem 4.44.
- Proposition 4.45 — is exactly the intersection of all measurable linear subspaces of full measure.
Significance
The Cameron–Martin theorem is what makes the Cameron–Martin space a canonical object rather than a formal construction: is simultaneously the set of admissible shifts, the intersection of all full-measure linear subspaces (Proposition 4.45), and the space whose unit ball governs Gaussian isoperimetry (Theorem 4.53, Borell–Sudakov–Cirel'son). Downstream in the notes it is used to identify invariant measures of linear SPDEs and to compare them; outside the notes it is the starting point of Malliavin calculus and of large deviation theory for Gaussian measures.
Status, precisely. The Mathlib library pinned by this mission already contains a substantial part of Section 4: the predicate IsGaussian (Definition 4.4), uniqueness of measures with equal characteristic functionals on a separable Banach space (Propositions 4.8 and 4.11), invariance of under rotations (Proposition 4.12), Fernique's theorem (Theorem 4.13), and the covariance form of (4.2) together with its boundedness (Corollary 4.14) as a continuous bilinear form on the dual. Those results are therefore not milestones here; they are the assumed foundation. What is absent, and what this mission asks for, is everything from the Cameron–Martin space onwards: its definition, its elementary properties, and Theorem 4.44 itself. No machine-checked proof of the infinite-dimensional Cameron–Martin theorem is known to the captain in any Lean library.
Difficulty
The naive route — write down the two densities and take their ratio — is unavailable: there is no translation-invariant reference measure on an infinite-dimensional Banach space, so "the density of " does not exist and the Radon–Nikodym derivative of with respect to must be produced directly, as the exponential of a random variable.
That random variable is the obstruction. For the functional is continuous and the computation is a characteristic-function identity. But is in general strictly smaller than : a general has an associated that exists only as an -limit of continuous functionals, defined -almost everywhere and linear only on a measurable subspace of full measure (Propositions 4.34 and 4.39). Establishing that these limits are Gaussian with the expected variance (Proposition 4.40) is the technical bridge, and it is why milestone 3 is stated as a statement about -limits rather than about elements of .
The converse half has a different shape. One must produce, for , a single one-dimensional projection that separates from arbitrarily well; unboundedness of over the covariance unit ball supplies with and as large as desired, and the quantitative Gaussian total-variation bound of milestone 5 converts this into total variation distance , i.e. mutual singularity.
Formalization scope
The development is in Lean 4 with Mathlib, in the namespace HairerSPDE, shared by the whole series drawn from these notes. The conventions it commits to:
- carries
NormedAddCommGroup,NormedSpace ℝ, its Borel σ-algebra,CompleteSpaceandSecondCountableTopology— the last two encode "separable Banach space". - Gaussianity is Mathlib's
IsGaussian, which is Definition 4.4 verbatim; centredness is the extra hypothesis , needed becauseIsGaussianpermits a non-zero mean. - The covariance form is Mathlib's
covarianceBilinDual, which equals (4.2) for centred measures with finite second moment and is set to zero otherwise; Fernique's theorem rules the degenerate branch out for Gaussian measures. - The Cameron–Martin norm is the -valued supremum above, so membership in is finiteness of that supremum; this is the only new definition the mission publishes.
- Translation is
fun x ↦ x + h, absolute continuity is Mathlib's≪, and "measurable linear subspace" is aSubmodule ℝ Bwhose carrier is a measurable set.
The goal is an equivalence, so neither half can be discharged vacuously: the direction is non-trivial already for in finite dimensions, and the converse has content precisely when . Note that always, and that for a Dirac mass the covariance form vanishes and ; both degenerate cases are inside the statement rather than excluded by hypothesis.
Contributions welcome beyond the milestones: the reproducing kernel space and the isomorphism of Proposition 4.34, measurable linear extensions (Proposition 4.39), the dilation singularity of Proposition 4.43, and in the infinite-dimensional case (second half of Proposition 4.45). All of these are reusable outside this mission.
Selected references
- M. Hairer, An Introduction to Stochastic PDEs, lecture notes, 2009/2023. arXiv:0907.4178
- V. I. Bogachev, Gaussian Measures, Mathematical Surveys and Monographs 62, American Mathematical Society, 1998. DOI:10.1090/surv/062
- X. Fernique, Intégrabilité des vecteurs gaussiens, C. R. Acad. Sci. Paris Sér. A-B 270 (1970), A1698–A1699.
- G. Da Prato, J. Zabczyk, Stochastic Equations in Infinite Dimensions, Cambridge University Press, 1992. DOI:10.1017/CBO9780511666223